potential function

Tags: #definition

potential function

Given an electrical network G=(V,E), a potential function U:VR is an assignment such that for all uev, Ve=UvUe, defined up to scaling by a constant.
The existence of such a function is equivalent to Kirchoff's second law

The nice thing about this formulation is that it's independent of direction.

Ohm's law then may be rewritten as

Ie=UvUuRe

and the first law is equivalent to for all vertices vi connected to v for v not connected to the battery

iUvUviRi=0

We can combine all the Uv terms together to get

(1R1++1Rd)UviUviRi=0

If v=1, then this would be equal to Ibat
If v=n, then this would be equal to Ibat

Connection to Kirchoff's matrix

The first law is equivalent to saying that for U the vector of all potentials U=[U1,,Un]T

KU=[Ibat00Ibat]$$where$K$is[[Zettelkasten/Unfiled/KirchoffsmatrixofanelectricalnetworkKirchoffsmatrixofanelectricalnetwork]].However,$K$isdegenerateastherearemanysolutionsfor$U$uptoscaling.Thus,we"ground"thenetworkbysetting$Un=0$.

\tilde{K} \begin{bmatrix}
U_1 \
\vdots \
U_{n-1}
\end{bmatrix} = \begin{bmatrix}
I_{bat} \
0 \
\vdots \
0
\end

where$K~$isthe[[Zettelkasten/Unfiled/reducedLaplacianmatrixreducedLaplacianmatrix]](asweremovedthe$n$throwandcolumn).Furthermore,wecanmaketheadditionalsimplifyingassumptionthat$Ibat=1$,thenrescaleafterwards.Then,notethatthe[[Zettelkasten/Unfiled/effectiveresistanceeffectiveresistance]]isthengivenby$U1$,ofwhichwemaysolvewith[[Zettelkasten/Unfiled/CramersruleCramersrule]].